trace ancillary: a highly-segmented silicon-pad detector ... · in beam test: silicon ancillary...
TRANSCRIPT
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
TRACE ancillary:a highly-segmented silicon-pad detector
for light charged particles emitted indirect nuclear reactions
Daniele MengoniUniversità e Sezione INFN di Padova
ITALIA
DREB07, RIKEN, JapanMay 30 ÷ June 2, 2007
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Outline
1 Introduction
2 TRACE simulation and designEstimations, simulation and performances evaluationSignals induced in silicon
3 Experimental testsIn beam test: silicon ancillary coupled to the AGATA clusterDetector & electronics (NIM, ASIC) tests
4 Conclusion
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Introduction
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
IntroductionInstrumentation: γ-spectrometers
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
IntroductionInstrumentation: ancillaries used in conjunction with γ-spectrometers
Selectivity improvement and background reduction
PRISMA
DANTE
MICROBALL
TIARAMUST2
EUCLIDES
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
IntroductionSuitable reactions
Direct nuclear reactionsin inverse kinematics to measure the angle of the recoiling lightparticle.
... Fusion-evaporation reactionsto measure energy and angle of the recoiling light particle withancillary detectors coupled with gamma arrays.
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
IntroductionSuitable reactions
Direct nuclear reactionsin inverse kinematics to measure the angle of the recoiling lightparticle.
... Fusion-evaporation reactionsto measure energy and angle of the recoiling light particle withancillary detectors coupled with gamma arrays.
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
Material Transparency, energy resolution,properties, costs
Particle discriminationtechnique
Segmentation
Efficiency
Pad (or strips)
4π detector
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
MaterialParticle discriminationtechnique E-∆E, thickness
Segmentation
Efficiency
Pad (or strips)
4π detector
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
Material
Particle discriminationtechniqueSegmentation Angular resolution
Efficiency
Pad (or strips)
4π detector
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
Material
Particle discriminationtechnique
SegmentationEfficiency Solid angle coverage, lowenergy threshold
Pad (or strips)
4π detector
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
Material
Particle discriminationtechnique
Segmentation
EfficiencyPad (or strips) Sizable number, heatdissipation, energy resolution
4π detector
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Design criteria
Guidelines
Material
Particle discriminationtechnique
Segmentation
Efficiency
Pad (or strips)4π detector Reaction kinematics
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: frameworkEvent generator, radiation interaction, filter (PSA, tracking), data collection (matricesand spectra)
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Simulation: TRACETRacking Array for light Charged particle Ejectiles
Starting point: improvement of the EUCLIDES Si ball;
Next steps: increase segmentation and solid anglecoverage without losing in simplicity (barrel, end-caps).
Hodoscope Euclides-like TRACE4,6,8module
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Transparency
Full-energy eff.:probability to detect the total energy of any emittedphoton individually
Peak-to-total ratio: the ratio of full energy efficiency to the totalinteraction efficiency.
Absolute photopeak eff. (%)
15
20
25
30
35
40
45
50
0 500 1000 1500 2000 2500 3000
Absolute photopeak eff. (%)
Energy (keV)
A180A180+Al chamber+EUCLIDESA180+Al chamber+TRACE4A180+Al chamber+TRACE6A180+Al chamber+TRACE8
Peak-to-total ratio (%)
0
20
40
60
80
100
0 500 1000 1500 2000 2500 3000
Peak-to-total ratio (%)
Energy (keV)
A180A180+Al chamber+EUCLIDES
A180+Al chamber+TRACE4+ASICsA180+Al chamber+TRACE6A180+Al chamber+TRACE8
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Doppler correctionTRACE8
Doppler broadening
uncertainty in the photon emission angle
uncertainty in the recoil energy
intrinsic detector resolution
2
2.5
3
3.5
4
4.5
5
5.5
6
6.5
0 1 2 3 4 5 6 7 8
FWHM (keV)
Segmentation (mm2)
transfer v/c=6.4%transfer v/c=7.8%
0
0.2
0.4
0.6
0.8
1
1.2
0 20 40 60 80 100 120 140 160 180
∆Eγ/E
γ (%)
Angle (deg)
∆θ = 0.5°∆β = 1%
v/c=15%v/c=10%v/c= 5%
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Collecting electrodesRear side current signals as a function of the injected particles.The particles are injected in the middle of the central pad.
α family3_MeV 5_MeV 10_MeV 30_MeV
Time (s)
1e−10 1e−09 1e−08 1e−07 1e−06 1e−05
Cu
rre
nt
(A)
2e−05
4e−05
6e−05
8e−05
1e−04
proton family3_MeV 5_MeV 10_MeV 30_MeV
Time (s)
1e−10 1e−09 1e−08 1e−07 1e−06 1e−05
Cu
rre
nt
(A)
1e−04
2e−04
3e−04
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Neighbour electrodesRear side, bipolar transient signals as a function of the injected particles.The particles are injected in the middle of the central pad.
α family3_MeV 5_MeV 10_MeV 30_MeV
Time (s)
1E−10 1E−9 1E−8 1E−7 1E−6 1E−5
Cu
rre
nt
(A)
−3e−06
−2e−06
−1e−06
0
proton family30_MeV 10_MeV 5_MeV 3_MeV
Time (s)
1E−10 1E−9 1E−8 1E−7 1E−6 1E−5
Cu
rre
nt
(A)
−2e−06
0
2e−06
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Ancillary impactSingle hit on Si, Ge cluster
Silicon center, PSA on Ge detector
Full information on the DSSSD, PSA on Ge detector
AGATA cluster + ancillary 49Ti Energy resolution
1365 1370 1375 1380 1385 1390 1395
1000
2000
3000
4000
5000
6000
E_titleCLUSTCORRCAL_pSIpGE
6.1 keV7.7 keV
Cou
nts
keV
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Preliminary tests: ITC-IRST detectors300 µm,1 mm, 1.5 mm thickness, 1x1, 2x2, 4x4 mm2, low resistivity, AC coupling.
Junction side: DC, AC pad; biasand reference voltage; guardrings; “punch-through” resistance.
pad layout zoom
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Preliminary tests: ITC-IRST detectorsEnergy resolution with modular NIM and ASIC electronics
0
50
100
150
200
250
300
350
400
450
4800 5000 5200 5400 5600 5800 6000 6200
Counts
Energy (keV)
50 keV
0
2000
4000
6000
8000
10000
12000
4800 5000 5200 5400 5600 5800 6000 6200
Counts
Energy (keV)
60 keV
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
ConclusionTelescope Prototype
ASIC: quasi-parallel energy-time cycle;
Telescope prototype closely resembles the traditional Sitelescope;
TRACE prototype key features: Si-pad technology,integrated electronics, high segmentation, PSA ...
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Summary
Simple estimations
Geometry simulation
PSA simulation
Ancillary impact
Si and electronics test
=⇒ telescope specifications and possible prototype.
Future perspectives:PSA testIn beam test
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Introduction TRACE simulation and design Experimental tests Conclusion Summary Acknowledgements
Acknowledgements
INFN (Italy)
LNL: A. Gadea, G. Prete, G. de Angelis, J.J. Valiente-Dobon,R. Orlandi, F. della Vedova, E. Sahin, R.P. Singh, R. Ponchia,P. Cocconi, D. Rosso.
Sezione di Padova: F. Recchia, E. Farnea, D.Bazzacco,S.Lunardi, C. Ur, R. Isocrate.
Sezione di Perugia: E. Fiandrini, G. Ambrosi, M. Ionica,G. Alberti.
IN2P3 (F)
C.M. Petrache, P. Edelbruck, L. Lavergne, L. Leterrier, and theMUST2 team.
Surrey University (UK)
P.H. Regan and the TIARA team.